Method and device for quantifying viscoelasticity of a medium

ABSTRACT

A method for quantifying viscoelasticity of a medium includes: obtaining a position-time graph of vibration propagation after the medium is subjected to a vibration excitation, determining an angle with maximum signal energy in the position-time graph by using angle projection, where the angle with the maximum signal energy corresponds to a slope of the position-time graph and the slope of the position-time graph is the propagation velocity of the vibration in the medium. Since the propagation velocity of the vibration in the medium is related to the viscoelasticity of the medium, a viscoelasticity parameter of the medium can be quantitatively calculated after the slope of the position-time graph is obtained. The method does not need to select a feature point from the position-time graph to calculate the slope of the position-time graph, and can efficiently and accurately quantifies viscoelasticity of the medium.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of International Application No.PCT/CN2018/088405, filed on May 25, 2018, which claims priority toChinese Patent Application No. 201710649552.9, filed on Jul. 21, 2017.The disclosures of the aforementioned applications are herebyincorporated by reference in their entireties.

TECHNICAL FIELD

The present disclosure relates to the technical field of measurement,and in particular, to a method and a device for quantifyingviscoelasticity of a medium.

BACKGROUND

When performing a vibration excitation on a medium, propagationcharacteristics of the vibration in the medium are related to theviscoelasticity of the medium. By measuring the propagationcharacteristics of the vibration, the viscoelasticity of the medium canbe quantified.

The above principle has been applied to many technical fields atpresent. Taking medical testing as an example, when testing organs ortissues such as liver, thyroid, and muscle, lesions can be located byquantifying the viscoelasticity of the medium.

Therefore, how to perform efficient and accurate viscoelasticityquantification of the medium is a problem to be solved.

SUMMARY

Embodiments of the present disclosure provide a method and a device forquantifying viscoelasticity of a medium. In order to have a basicunderstanding of some aspects of the disclosed embodiments, a briefsummary is given below. This summary is neither a general review, norintended to determine key/important constituent elements or to describethe protection scope of these embodiments. Its sole purpose is topresent some concepts in a simplified form as a prelude of the followingdetailed description.

According to a first aspect of the embodiments of the presentdisclosure, a method for quantifying viscoelasticity of a medium isprovided, and the method includes:

obtaining a position-time graph of vibration propagation after themedium is subjected to a vibration excitation;

performing angle projection along each angle within a preset angle rangeon the position-time graph to determine a slope of the position-timegraph corresponding to an angle with maximum signal energy; and

obtaining a viscoelasticity parameter of the medium according to theslope.

Based on the method, as a first optional embodiment, the performingangle projection along each angle within a preset angle range on theposition-time graph to determine a slope of the position-time graphcorresponding to an angle with maximum signal energy, includes:

performing integral calculation along each angle within the preset anglerange on the position-time graph;

determining an angle with a maximum integral value as a slope angle of aslope line of the position-time graph; and

determining a slope of the slope line using the slope angle.

Based on the method, as a second optional embodiment, the performingangle projection along each angle within a preset angle range on theposition-time graph to determine a slope of the position-time graphcorresponding to an angle with maximum signal energy, includes:

calculating a gray-level co-occurrence matrix along each angle withinthe preset angle range for the position-time graph;

obtaining an image texture feature for each angle;

determining the angle with the maximum signal energy as a slope angle ofa slope line of the position-time graph, using the image texturefeature; and

determining a slope of the slope line using the slope angle.

Based on the method, the first embodiment, or the second embodiment, asa third optional embodiment, the method further includes:

filtering out reflected waves in the position-time graph before theangle projection.

Based on the third embodiment, as a fourth optional embodiment, thefiltering out reflected waves in the position-time graph, includes:performing direction filtering on the position-time graph.

Based on the method, the first embodiment, or the second embodiment, asa fifth optional embodiment, the obtaining a position-time graph ofvibration propagation, includes:

obtaining the position-time graph of the vibration propagation along aset vibration propagation direction.

According to a second aspect of the embodiments of the presentdisclosure, a device for quantifying viscoelasticity of a medium isprovided, and the device includes:

an image module, configured to obtain a position-time graph of vibrationpropagation after the medium is subjected to a vibration excitation;

a determining module, configured to perform angle projection along eachangle within a preset angle range on the position-time graph todetermine a slope of the position-time graph corresponding to an anglewith maximum signal energy; and

a quantifying module, configured to obtain a viscoelasticity parameterof the medium according to the slope.

Based on the device, as a first optional embodiment, the determiningmodule includes:

a calculating sub-module, configured to perform integral calculation onthe position-time graph along each angle within the preset angle range;

a determining sub-module, configured to determine an angle with amaximum integral value calculated by the calculating sub-module as aslope angle of a slope line of the position-time graph; and determine aslope of the slope line using the slope angle.

Based on the device, as a second optional embodiment, the determiningmodule includes:

a calculating sub-module, configured to calculate a gray-levelco-occurrence matrix along each angle within the preset angle range forthe position-time graph;

a determining sub-module, configured to obtain an image texture featureof each angle; determine the angle with the maximum signal energy as aslope angle of a slope line of the position-time graph, using the imagetexture feature; and determine a slope of the slope line using the slopeangle.

Based on the device, the first embodiment, or the second embodiment, asa third optional embodiment, the device further includes:

a filtering module, configured to filter out reflected waves in theposition-time graph before the angle proj ection.

Based on the device, the first embodiment, or the second embodiment, asa fourth optional embodiment, the image module obtains the position-timegraph of the vibration propagation along a set vibration propagationdirection.

According to a third aspect of the embodiments of the presentdisclosure, a device for quantifying viscoelasticity of a medium isprovided, and the device includes:

a memory, storing execution instructions;

a processor, configured to read the execution instructions to accomplishthe following operations:

obtaining a position-time graph of vibration propagation after themedium is subjected to a vibration excitation;

performing angle projection along each angle within a preset angle rangeon the position-time graph to determine a slope of the position-timegraph corresponding to an angle with maximum signal energy; and

obtaining a viscoelasticity parameter of the medium according to theslope.

The technical solutions provided by the embodiments of the presentdisclosure may include the following beneficial effects:

the angle with the maximum signal energy in the position-time diagram isdetermined using the angle projection, the angle with the maximum signalenergy corresponds to the slope of the position-time graph, and theslope of the position-time graph is the propagation velocity of thevibration in the medium. Since the propagation velocity of the vibrationin the medium is related to the viscoelasticity of the medium, theviscoelasticity parameter of the medium can be quantitatively calculatedafter the slope of the position-time graph is obtained. The embodimentsof the present disclosure do not need to select feature points from theposition-time graph to calculate the slope of the position-time graph,and is not affected by noise and has a small calculation amount, and canefficiently and accurately quantifies the viscoelasticity of the medium.

It should be understood that the above general description and thefollowing detailed description are merely exemplary and explanatory, andshould not limit the present disclosure.

BRIEF DESCRIPTION OF DRAWINGS

The drawings herein are incorporated in and constitute a part of thepresent specification, illustrating the embodiments consistent with thepresent disclosure, and serving to explain the principles of the presentdisclosure together with the description.

FIG. 1 shows a flow chart of a method for quantifying viscoelasticity ofa medium according to an exemplary embodiment;

FIG. 2 shows a flow chart of a method for quantifying viscoelasticity ofa medium according to an exemplary embodiment;

FIG. 3 shows a flow chart of a method for quantifying viscoelasticity ofa medium according to an exemplary embodiment;

FIG. 4 shows a block diagram of a device for quantifying viscoelasticityof a medium according to an exemplary embodiment;

FIG. 5 is a block diagram of a determining module shown in FIG. 4 ;

FIG. 6 shows a block diagram of a device for quantifying viscoelasticityof a medium according to an exemplary embodiment; and

FIG. 7 shows a block diagram of a device for quantifying viscoelasticityof a medium according to an exemplary embodiment.

DESCRIPTION OF EMBODIMENTS

The following description and the drawings sufficiently illustratespecific embodiments of the present disclosure to enable those skilledin the art to practice them. The embodiments represent only possiblevariations. Unless otherwise explicitly required, individual componentsand functions are optional, and the order of operations may be varied.Parts and features of some embodiments may be included in or replaceparts and features of other embodiments. The scope of embodiments of thepresent disclosure includes the entire scope of the claims, and allavailable equivalents of the claims. Herein, the various embodiments maybe individually or collectively represented by the term “invention”,which is for convenience only, and if more than one invention isactually disclosed, it is not intended to automatically limit the scopeof the application to any single invention or inventive concept. Herein,relational terms such as first and second are used only to distinguishone entity or operation from another entity or operation, and do notrequire or imply that there is any actual relationship or order betweenthese entities or operations. Moreover, the terms “including”,“containing” or any other variation thereof are intended to encompassnon-exclusive inclusion, such that processes, methods, or devices thatinclude a series of elements include not only those elements, but alsoother elements not explicitly listed. The various embodiments herein aredescribed in a progressive manner, each embodiment focuses on thedifferences from other embodiments. For the same and similar partsbetween the various embodiments, reference can be made to each other. Asfor the structures and products or the like disclosed in theembodiments, since they correspond to the parts disclosed in theembodiments, the description is relatively simple, and reference can bemade to the description of the method part for the relevant parts.

FIG. 1 shows a flow chart of a method for quantifying viscoelasticity ofa medium according to an exemplary embodiment. As shown in FIG. 1 , themethod includes the following steps.

In step 11, obtaining a position-time graph of vibration propagationafter the medium is subjected to a vibration excitation.

In step 12, performing angle projection along each angle within a presetangle range on the position-time graph to determine an angle withmaximum signal energy, which corresponds to a slope of the position-timegraph.

The preset angle range refers to an angle range for performing the angleprojection selected according to actual situations. As an optionalimplementation, the preset angle range may be 360 degree, andaccordingly a full-angled angle projection is required to be performed.As another optional implementation, the angle range for performing theangle projection is selected according to the characteristics of theobtained position-time graph. The horizontal axis of the position-timegraph obtained in step 11 indicates time and the vertical axis indicatesposition. If the vibration propagates to a distant place only from thestarting point of the vibration excitation, when the velocity ofvibration propagation is infinitely large, it is close to a straightline parallel to the vertical axis on the position-time graph, and whenthe velocity of the vibration propagation is infinitely small, it isclose to a straight line parallel to the horizontal axis on theposition-time graph. At this time, a preset angle range of 90 degree canmeet the needs, without the need to perform full-angle projection, andthen the efficiency of quantifying the viscoelasticity of the medium isimproved. If the vibration can also continue to propagate in an oppositedirection besides propagating to the distant place from the startingpoint of the vibration excitation, the preset angle range may be 180degree. As for the actual starting point and ending point of the presetangle range, with the rectangular coordinate system remaining unchanged,it is related to the starting point of 0 degree and the counterclockwiseor clockwise rotation direction, which can be selected as needed, aslong as the preset angle range is guaranteed.

Each angle refers to each angle within the preset angle range alongwhich the angular projection is performed. The selection of specificangle is determined according to a time accuracy requirement and acalculation speed requirement. The higher the time accuracy requirementis, the higher the accuracy requirement of angle selection is; and thehigher the calculation speed requirement is, the lower the accuracyrequirement of angle selection is. For example, it can be selected from0.01 degree to 1 degree.

The angle projection refers to performing image feature recognition orextraction on set angles to determine an angle with the maximum signalenergy.

In step 13, obtaining a viscoelasticity parameter of the mediumaccording to the slope.

The viscoelasticity parameter includes at least one of a viscosityparameter and an elastic parameter.

The slope of the position-time graph is determined by a distance ofvibration propagation per unit time, that is, the velocity of thevibration propagation in the medium. In a homogeneous medium, thevelocity of vibration propagation is related to the viscoelasticity ofthe medium. The viscoelasticity parameter of the medium can bequantitatively calculated after the slope of the position-time graph isobtained. Therefore, how to efficiently and accurately obtain the aboveslope becomes a key of quantifying the viscoelasticity of the medium. Inthe present exemplary embodiment, the angle with the maximum signalenergy is determined using the angle projection. Since the angle withthe maximum signal energy corresponds to the slope of the position-timegraph, that is, it is equivalent to obtain the slope of theposition-time graph. This method does not need to select a peak, atrough, or a certain phase of vibration from the position-time graph asa feature point to calculate the slope of the position-time graph. It isnot affected by noise and has a small calculation amount. It is anefficient and accurate method for quantifying the viscoelasticity of themedium.

In an exemplary embodiment, after performing the vibration excitation onthe medium through mechanical vibration, acoustic radiation force, orother manners capable of generating vibration, the medium generatesvibration, and the vibration propagates in the medium. Due to thelimited propagation velocity of the above vibration in the medium, adetection wave can be used to perform dynamic imaging for the medium.The above detection wave may be a light wave, an ultrasonic wave, or thelike. The above dynamic imaging may be one-dimensional imaging,two-dimensional imaging, or three-dimensional imaging.

When the above-mentioned vibration propagates in the medium, thewave-front will reach different positions along the propagationdirection at different times. The echo signal generated for the imagingof the medium by the detection wave will undergo phase decorrelation.Utilizing this characteristic of phase decorrelation, motion informationof the medium can be obtained through algorithms such ascross-correlation, autocorrelation, and optical flow. The position-timegraph can be obtained along the set vibration propagation direction. Theabove algorithms may be various methods based on block matching ornon-block matching. The above set vibration propagation direction is anactual propagation direction of the vibration when the vibrationpropagates in only one propagation direction, and is a selectedpropagation direction when the vibration propagates in multiplepropagation directions. For example, when the medium is a uniform sheet,after the medium is excited by vibration, the vibration will propagatealong the extension direction of the sheet, and the set vibrationpropagation direction at this time is an actual propagation direction ofthe vibration. For another example, when the medium has a stereoscopicirregular shape, the wave-front of the vibration propagation has athree-dimensional shape (for example, the wave-front of the vibrationpropagation is an ellipsoid), then different position-time graphs areobtained along different vibration propagation directions, and the setvibration propagation direction at this time is a selected propagationdirection of interest. The above-mentioned propagation direction ofinterest is determined according to a direction that needs to beactually measured, for example, it may be at least one of a direction inwhich the vibration propagates fastest, a direction in which thevibration propagates slowest, and a direction in which the velocity ofthe vibration propagation is within a certain range.

In an exemplary embodiment, when the vibration propagates in the medium,reflected waves are generated when the vibration encounters edges of themedium or foreign objects. To improve the accuracy of subsequentprocessing, as shown in FIG. 2 , before performing the angle projection,the method may also include step 11′, that is, filtering out thereflected waves in the position-time graph. There are many ways tofilter out, and direction filtering is one implementation of them.

In an exemplary embodiment, determining the angle with the maximumsignal energy through the angle projection, and then obtaining the slopeof the position-time graph, can be implemented through integralcalculation. For example, integral calculation is performed along eachangle within the preset angle range on the position-time graph. When anintegral angle is consistent with the vibration propagation direction,the energy is gathered, and the obtained integral value at this time ismaximum. Therefore, the angle with the maximum integral value isdetermined as the slope angle of the slope line of the position-timegraph. The slope of the slope line of the position-time graph can beobtained according to the obtained slope angle, combined with positionand time information. The above integral calculation is also referred toas Radon transform.

In an exemplary embodiment, since an image texture feature can beobtained by calculating a gray-level co-occurrence matrix, and the imagetexture feature can reflect the magnitude of the signal energy, thegray-level co-occurrence matrix can be used to obtain information of theangle with the maximum signal energy. Based on the above principle,determining the angle with the maximum signal energy through the angleprojection, and then obtaining the slope of the position-time graph, canbe implemented by calculating the gray-level co-occurrence matrix. Forexample, for the position-time graph, a gray-level co-occurrence matrixis first calculated along each angle within the preset angle range.Then, the image texture feature of each angle is obtained using thegray-level co-occurrence matrix. Then, the angle with the maximum signalenergy is determined as the slope angle of the slope line of theposition-time graph by using the image texture feature. Finally, theslope angle is determined using the slope angle.

According to the principle of mechanics, the viscoelasticity of themedium determines the propagation velocity of the vibration therein.Therefore, the propagation velocity of the vibration in the medium canbe learned by obtaining the slope of the position-time graph. And thenthe viscoelasticity parameter of the medium can be quantitativelyobtained according to the principle of mechanics. The viscoelasticityparameter here may include shear modulus, Young's modulus, shearviscoelasticity, shear viscosity, mechanical impedance, mechanicalrelaxation time, anisotropy, and the like.

The application of the method for quantifying viscoelasticity of amedium in the embodiments of the present disclosure will be given in aspecific application scenario.

When a non-destructive viscoelasticity testing is performed on aviscoelastic medium such as human liver, the viscoelasticity of themedium needs to be quantified. A testing apparatus includes an excitingdevice and an imaging device, where the exciting device performs avibration excitation on the medium to be detected, and the imagingdevice utilizes ultrasound to perform imaging for the medium after thevibration excitation. When the vibration propagates in the medium, thewave-front will reach different positions along the propagationdirection at different times, forming a position-time graph. The abovewave-front may be one of a peak, a trough, or the same phase ofvibration.

As shown in FIG. 3 , the method for quantifying viscoelasticity of amedium in this specific application scenario may include the followingsteps.

In step 31, performing a vibration excitation on the medium.

In step 32, performing dynamic imaging for the medium using ultrasound.

In step 33, obtaining a position-time graph of vibration propagationfrom the imaging of the medium.

In step 34, performing direction filtering on the position-time graph.

In step 35, performing a Radon transform to determine a slope of theposition-time graph.

In step 36, calculating a viscoelasticity parameter of the mediumaccording to the determined slope and principle of mechanics.

In various exemplary embodiments of the above method for quantifyingviscoelasticity of a medium, when there are at least two set vibrationpropagation directions, one position-time graph is obtained for each setvibration propagation direction correspondingly, and then theviscoelasticity parameter of the medium corresponding to theposition-time graph is obtained. By synthesizing the obtained at leasttwo sets of viscoelasticity parameters, the viscoelasticity of themedium can be evaluated more comprehensively.

The various exemplary embodiments of the method for quantifyingviscoelasticity of a medium given above may be combined according tocircumstances, and the combination relationship between the variousexemplary embodiments is not limited here.

FIG. 4 is a block diagram of a device for quantifying viscoelasticity ofa medium according to an exemplary embodiment. The device may be locatedin a control host of an apparatus for testing viscoelasticity of amedium, for example, in a control host of a non-destructive testingapparatus for liver in the medical testing field. The device can also belocated in a cloud, and testing data of the apparatus for testingviscoelasticity of a medium needs to be processed in the cloud.

The device shown in FIG. 4 includes an image module 41, a determiningmodule 42 and a quantifying module 43.

The image module 41 is configured to obtain a position-time graph ofvibration propagation after the medium is subject to a vibrationexcitation.

The determining module 42 is configured to perform angle projectionalong each angle within a preset angle range on the position-time graphto determine an angle with maximum signal energy. The angle with themaximum signal energy described above corresponds to a slope of theposition-time graph.

The quantifying module 43 is configured to obtain a viscoelasticityparameter of the medium according to the slope of the position-timegraph.

In an exemplary embodiment, as shown in FIG. 5 , the determining module42 employs a Radon transform to perform the angle projection anddetermines the angle with the maximum signal energy. At this time, thedetermining module 42 includes a calculating sub-module 421 and adetermining sub-module 422.

The calculating sub-module 421 is configured to perform integralcalculation along each angle within the preset angle range on theposition-time graph.

The determining sub-module 422 is configured to determine an angle witha maximum integral value calculated by the calculating sub-module 421 asa slope angle of a slope line of the position-time graph; and determinea slope of the slope line of the position-time graph through the slopeangle.

As an optional implementation, when a gray-level co-occurrence matrix isused to determine the slope angle, the calculating sub-module 421 may beconfigured to calculate the gray-level co-occurrence matrix along eachangle within the preset angle range for the position-time graph. Thedetermining sub-module 422 may be configured to obtain an image texturefeature of the each angle; determine the angle with the maximum signalenergy as a slope angle of a slope line of the position-time graph usingthe image texture feature; and determine a slope of the slope line usingthe slope angle.

In an exemplary embodiment, as shown in FIG. 6 , the device forquantifying viscoelasticity of a medium further includes: a filteringmodule 44, configured to filter out reflected waves in the position-timegraph before the determination module 42 performs the angle projection.

In an exemplary embodiment, the image module 41 obtains theposition-time graph of the vibration propagation along a set vibrationpropagation direction.

The application of the device for quantifying viscoelasticity of amedium in the embodiments of the present disclosure is given in aspecific application scenario.

When performing a non-destructive viscoelasticity testing on aviscoelastic medium such as human liver, the viscoelasticity of themedium needs to be quantified. A testing apparatus includes an excitingdevice and an imaging device, where the exciting device performs avibration excitation on the medium to be detected, and the imagingdevice utilizes ultrasound to perform imaging for the medium after thevibration excitation.

When the vibration propagates in the medium, the wave-front will reachdifferent positions along the propagation direction at different times,forming a position-time graph. The above wave-front may be one of apeak, a trough, or the same phase of vibration. The device forquantifying viscoelasticity of a medium obtains the position-time graphof the vibration propagation from the imaging of the medium along theset propagation direction. Then the device for quantifyingviscoelasticity of a medium performs integral calculation along eachangle on the position-time graph, and determines the angle with themaximum integral value as the slope angle of the slope line of theposition-time graph, and then determines the slope of the position-timegraph. Finally, the device for quantifying viscoelasticity of a mediumcalculates and obtains the viscoelasticity parameter of the mediumaccording to the determined slope and principle of mechanics.

FIG. 7 is a block diagram of a device for quantifying viscoelasticity ofa medium according to an exemplary embodiment. The device may be locatedin a control host of an apparatus for testing viscoelasticity of amedium, for example, in a control host of a non-destructive testingapparatus for liver in the medical testing field. The device can also belocated in a cloud, and testing data of the apparatus for testingviscoelasticity of a medium needs to be processed in the cloud.

The various exemplary embodiments of the device for quantifyingviscoelasticity of a medium given above may be combined according tocircumstances, and the combination relationship between the variousexemplary embodiments is not limited here.

The device shown in FIG. 7 includes: a memory 71 and a processor 72.

The memory 71 stores execution instructions.

The processor 72 is configured to read the execution instructions fromthe memory 71 to execute some or all steps in the exemplary embodimentsof the method for quantifying viscoelasticity of a medium describedabove. The processor 72 may be implemented by a chip.

If the device for quantifying viscoelasticity of a medium shown in FIG.7 is located in the control host of the apparatus for testingviscoelasticity of a medium, it can be connected to an exciting deviceand an imaging device in the apparatus for quantifying viscoelasticityof a medium by bus, wireless, etc. At this time, the device hasinterfaces to realize the above connections and correspondingcommunication mechanism.

If the device for quantifying viscoelasticity of a medium shown in FIG.7 is located in the cloud, it can communicate with the apparatus fortesting viscoelasticity of a medium through a network.

It should be understood that the present disclosure is not limited tothe processes and structures that have been described above and shown inthe drawings, and various modifications and changes can be made withoutdeparting from the scope thereof. The scope of the present disclosure isonly limited by the appended claims.

What is claimed is:
 1. A method for quantifying viscoelasticity of amedium, wherein the method comprises: generating, by an exciting device,a vibration excitation on the medium to make the medium generatevibration and make the vibration propagate in the medium; performing, byan imaging device, imaging for the medium after the vibration excitationis generated by virtue of a detection wave of the imaging device;obtaining, by the imaging device, a position-time graph of vibrationpropagation along a set vibration propagation direction from dynamicimaging of the medium, wherein a horizontal axis of the position-timegraph indicates time, and a vertical axis of the position-time graphindicates a position of wave-front of the vibration; performing angleprojection along directions having respective angles relative to apreset line of 0 degree on the position-time graph to determine a slopeof the position-time graph corresponding to an angle with maximum signalenergy, wherein the respective angles are within a preset angle range;and obtaining, according to the slope, propagation velocity of thevibration, and determining, according to principle of mechanics and thepropagation velocity of the vibration, a viscoelasticity parameter ofthe medium; wherein the performing the angle projection along thedirections having respective angles relative to the preset line of 0degree on the position-time graph to determine the slope of theposition-time graph corresponding to the angle with maximum signalenergy, comprises: performing integral calculation along each anglewithin the preset angle range on the position-time graph, wherein theintegral calculation is Radon transform; determining an anglecorresponding to a maximum integral value obtained by the Radontransform as a slope angle of a slope line of the position-time graph;and determining the slope of the slope line using the slope angle. 2.The method according to claim 1, wherein the method further comprises:filtering out reflected waves in the position-time graph before theperforming the angle projection.
 3. The method according to claim 2,wherein the filtering out the reflected waves in the position-timegraph, comprises: performing direction filtering on the position-timegraph.
 4. A device for quantifying viscoelasticity of a medium, whereinthe device comprises: a memory, storing execution instructions; and aprocessor, configured to read the execution instructions to: generate avibration excitation on the medium to make the medium generate vibrationand make the vibration propagate in the medium; perform imaging for themedium after the vibration excitation is generated by virtue of adetection wave of an imaging device; obtain a position-time graph ofvibration propagation along a set vibration propagation direction fromthe dynamic imaging of the medium, wherein a horizontal axis of theposition-time graph indicates time, and a vertical axis of theposition-time graph indicates a position of wave-front of the vibration;perform angle projection along directions having respective anglesrelative to a preset line of 0 degree on the position-time graph todetermine a slope of the position-time graph corresponding to an anglewith maximum signal energy, wherein the respective angles are within apreset angle range; and obtain, according to the slope, propagationvelocity of the vibration, and determine, according to principle ofmechanics and the propagation velocity of the vibration, aviscoelasticity parameter of the medium; wherein the processor isconfigured to read the execution instructions to: perform integralcalculation along each angle within the preset angle range on theposition-time graph, wherein the integral calculation is Radontransform; determine an angle corresponding to a maximum integral valueobtained by the Radon transform as a slope angle of a slope line of theposition-time graph; and determine the slope of the slope line using theslope angle.
 5. The device according to claim 4, wherein the processoris further configured to read the execution instructions to: filter outreflected waves in the position-time graph before performing the angleprojection.